Zoom lens and image pickup apparatus including the same

ABSTRACT

A zoom lens includes, in order from an object side to an image side: a first lens unit having a positive refractive power that does not move for zooming; a second lens unit having a negative refractive power that moves during zooming; a third lens unit having a positive refractive power that moves during zooming; and at least one lens unit having a positive refractive power, and focal lengths of the zoom lens at a wide angle end and a telephoto end, a maximum value of a half angle of field at the wide angle end, and products of lateral magnifications of lens units arranged on the image side of the third lens unit in a state in which focus is at infinity at the telephoto end and the wide angle end are appropriately set.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a zoom lens suitable for a television camera, a video camera, a film camera, a broadcasting television camera, and a movie camera, and more particularly, to a telephoto zoom lens having a large aperture and a high magnification.

2. Description of the Related Art

In a case where a nature program or the like is photographed for television (for example, an animal, a bird, or the like is photographed outdoors from a long distance), a zoom lens that is usable up to a focal length in a super telephoto range at a high magnification (for example, a high magnification of 7× or more and a half angle of field of 3 degrees or less at a telephoto end) and has high optical performance is required. In such photographing, a camera is often carried on a shoulder for photographing, and hence a zoom lens that is smaller in size and weight and has good portability is required. Moreover, in recent years, in addition to related-art video cameras and broadcasting television cameras, opportunities of photographing moving images are increasing as in a case where a camera for still photography, such as a single lens reflex camera, is also used for photographing a moving image. With a zoom lens for photographing a moving image, a zoom operation or a focus operation is performed during photographing, and hence in a case where a total lens length is changed at the time of the operation, an operation sound becomes noise to affect the photography, which is undesirable. Therefore, a demand for a zoom lens in which a first lens unit is fixed during zooming and which is of an inner focus type is increasing as a zoom lens suitable for moving image photography. In general, a size of a sensor (image pickup element) of the single reflex camera is larger than one inch, and is larger than a sensor having a size of one inch or less, which is mainly used in a video camera or a broadcasting television camera. Therefore, there is an increasing demand for the zoom lens having the high magnification and being usable in the super telephoto range, which is compatible with such a large sensor as to exceed one inch, good in portability and functionality, and suitable for moving image photography.

In Japanese Patent Application Laid-Open No. 2007-139858, there is proposed a telephoto zoom lens including four lens units, which has an angle of field of about 0.7 degrees at the telephoto end and a magnification of about 15×, and is suitable for a ⅔-inch broadcasting television camera.

In Japanese Patent Application Laid-Open No. 2004-085846, there is proposed a zoom lens including four lens units, which has an angle of field of about 1.6 degrees at the telephoto end and a magnification of about 3×.

In regard to the zoom lens described in Japanese Patent Application Laid-Open No. 2007-139858, as a problem in adapting to a still larger image pickup element and increasing a magnification while maintaining a large aperture ratio, an effective diameter on an image side of a zoom lens unit is increased, and hence the entire zoom lens is difficult to downsize.

In regard to the zoom lens described in Japanese Patent Application Laid-Open No. 2004-085846, as a problem in further increasing the magnification, a movement amount of a third lens unit for correcting an image plane is difficult to suppress, and in addition, a total lens thickness of a first lens unit is large, with the result that the entire zoom lens is difficult to downsize.

SUMMARY OF THE INVENTION

It is an object of the present invention to provide a zoom lens in which a paraxial refractive power arrangement of a first lens unit and a zoom lens unit is appropriately defined, which has a high magnification and is usable in a super telephoto range (for example, a high magnification of 7× or more and a half angle of field of 3 degrees or less at a telephoto end), and which is small in size and weight even in a case of adapting to a large sensor (for example, one inch or more).

In order to achieve the above-mentioned object, according to one embodiment of the present invention, there is provided a zoom lens, including, in order from an object side to an image side: a first lens unit having a positive refractive power that does not move for zooming; a second lens unit having a negative refractive power that moves during zooming; a third lens unit having a positive refractive power that moves during zooming; and at least one lens unit having a positive refractive power,

in which the following conditions are satisfied:

0.02<LN(|βct/βcw|)/LN(ft/fw)<0.50

2.0<ft/f1<7.0

20<ft/(fw×tan ωw)<120

where fw and ft represent focal lengths of the zoom lens at a wide angle end and a telephoto end, respectively, ωw represents a maximum value of a half angle of field at the wide angle end, βct and βcw represent products of lateral magnifications of lens units arranged on the image side of the third lens unit in a state in which focus is at infinity at the telephoto end and the wide angle end, respectively, and LN( ) in the conditional expression represents a natural logarithm of a numerical value in parentheses.

According to the one embodiment of the present invention, it is possible to achieve the zoom lens which has the high magnification and is usable in the super telephoto range (for example, the high magnification of 7× or more and the half angle of field of 3 degrees or less at the telephoto end), and which is small in size and weight even in the case of adapting to the large sensor (for example, one inch or more).

Further features of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a lens cross-sectional view in a state in which focus is at infinity at a wide angle end in a zoom lens according to Embodiment 1.

FIG. 2A is a longitudinal aberration diagram when focus is at infinity at the wide angle end in the zoom lens according to Embodiment 1.

FIG. 2B is a longitudinal aberration diagram when focus is at infinity at a focal length of 200 mm in the zoom lens according to Embodiment 1.

FIG. 2C is a longitudinal aberration diagram when focus is at infinity at a telephoto end in the zoom lens according to Embodiment 1.

FIG. 3 is a lens cross-sectional view when focus is at infinity at the wide angle end in a zoom lens according to Embodiment 2.

FIG. 4A is a longitudinal aberration diagram when focus is at infinity at the wide angle end in the zoom lens according to Embodiment 2.

FIG. 4B is a longitudinal aberration diagram when focus is at infinity at a focal length of 240 mm in the zoom lens according to Embodiment 2.

FIG. 4C is a longitudinal aberration diagram when focus is at infinity at the telephoto end in the zoom lens according to Embodiment 2.

FIG. 5 is a lens cross-sectional view when focus is at infinity at the wide angle end in a zoom lens according to Embodiment 3.

FIG. 6A is a longitudinal aberration diagram when focus is at infinity at the wide angle end in the zoom lens according to Embodiment 3.

FIG. 6B is a longitudinal aberration diagram when focus is at infinity at the focal length of 200 mm in the zoom lens according to Embodiment 3.

FIG. 6C is a longitudinal aberration diagram when focus is at infinity at the telephoto end in the zoom lens according to Embodiment 3.

FIG. 7 is a lens cross-sectional view when focus is at infinity at the wide angle end in a zoom lens according to Embodiment 4.

FIG. 8A is a longitudinal aberration diagram when focus is at infinity at the wide angle end in the zoom lens according to Embodiment 4.

FIG. 8B is a longitudinal aberration diagram when focus is at infinity at the focal length of 200 mm in the zoom lens according to Embodiment 4.

FIG. 8C is a longitudinal aberration diagram when focus is at infinity at the telephoto end in the zoom lens according to Embodiment 4.

FIG. 9 is a lens cross-sectional view when focus is at infinity at the wide angle end in a zoom lens according to Embodiment 5.

FIG. 10A is a longitudinal aberration diagram when focus is at infinity at the wide angle end in the zoom lens according to Embodiment 5.

FIG. 10B is a longitudinal aberration diagram when focus is at infinity at a focal length of 500 mm in the zoom lens according to Embodiment 5.

FIG. 10C is a longitudinal aberration diagram when focus is at infinity at the telephoto end in the zoom lens according to Embodiment 5.

FIG. 11 is a lens cross-sectional view when focus is at infinity at the wide angle end in a zoom lens according to Embodiment 6.

FIG. 12A is a longitudinal aberration diagram when focus is at infinity at the wide angle end in the zoom lens according to Embodiment 6.

FIG. 12B is a longitudinal aberration diagram when focus is at infinity at a focal length of 400 mm in the zoom lens according to Embodiment 6.

FIG. 12C is a longitudinal aberration diagram when focus is at infinity at the telephoto end in the zoom lens according to Embodiment 6.

FIG. 13 is a schematic diagram of a main part of an image pickup apparatus according to the present invention.

FIG. 14A is a schematic diagram of a paraxial refractive power arrangement of a first lens unit according to the present invention.

FIG. 14B is a schematic diagram of a paraxial refractive power arrangement of the first lens unit according to the present invention.

FIG. 15 is a schematic diagram regarding two-color chromatic aberration correction and a remaining secondary spectrum of a lateral chromatic aberration of a negative lens unit.

FIG. 16 is a schematic diagram regarding two-color chromatic aberration correction and a remaining secondary spectrum of a longitudinal chromatic aberration of a positive lens unit.

DESCRIPTION OF THE EMBODIMENTS

Now, embodiments of the present invention are described in detail with reference to the accompanying drawings. A zoom lens according to the present invention includes, in order from an object side to an image side, a first lens unit having a positive refractive power that does not move for zooming. The zoom lens also includes a second lens unit having a negative refractive power that moves during zooming, a third lens unit having a positive refractive power that moves during zooming, and at least one positive lens unit. The phrase “lens unit does not move for zooming” as used herein means that the lens unit is not driven for the purpose of performing zooming but may move for focusing in a case where the zooming and the focusing are performed at the same time.

With a zoom lens according to each embodiment, a relationship of a focal length of the first lens unit and a focal length of the entire zoom lens at a telephoto end, and a magnification sharing ratio of the second and subsequent lens units are appropriately defined to realize reduction in size and weight even in a case of adapting to a large sensor with a zoom lens which has a high magnification and is usable in a super telephoto range. Note that, a format of the sensor as used herein corresponds to a size of an imaging surface of an image pickup element, and generally has a diagonal length of 11 mm for a ⅔-inch sensor and 16 mm for a one-inch sensor.

More specifically, the zoom lens according to the present invention is a zoom lens including, in order from the object side to the image side, a first lens unit having a positive refractive power that does not move for zooming, a second lens unit having a negative refractive power that moves during zooming, a third lens unit having a positive refractive power that moves during zooming, and at least one positive lens unit. Moreover, the following conditions are satisfied:

0.02<LN(|βct/βcw|)/LN(ft/fw)<0.50  (1)

2.0<ft/f1<7.0  (2)

20<ft/(fw×tan ωw)<120  (3)

where fw and ft represent focal lengths of the zoom lens at a wide angle end and the telephoto end, respectively, ωw represents a maximum value of a half angle of field at the wide angle end, and βct and βcw represent products of lateral magnifications of the third lens unit and the subsequent lens units in a state in which focus is at infinity at the telephoto end and the wide angle end, respectively.

Note that, LN( ) in the conditional expression represents a natural logarithm of a numerical value in parentheses.

The conditional expression (1) defines a relationship of products βcw and βct of the lateral magnifications of the third lens unit and the subsequent lens units at the wide angle end and the telephoto end and ft/fw, which is a magnification of the zoom lens, and hence defines a magnification sharing ratio of the third lens unit and the subsequent lens units.

When LN(|βct/βcw|)/LN(ft/fw) in the conditional expression (1) exceeds an upper limit, the magnification sharing ratio of the third and subsequent lens units becomes too large. The third lens unit and the subsequent lens units are configured to have a weaker refractive power than the second lens unit, and hence movement amounts of the third and subsequent lens units become large for obtaining a predetermined magnification sharing ratio, which makes it difficult to reduce a total lens length. When LN(|βct/βcw|)/LN(ft/fw) in the conditional expression (1) falls below a lower limit, a movement amount of the second lens unit, which is a main zoom lens unit, becomes too large, with the result that variations in lateral chromatic aberration and image plane aberration generated in the second lens unit become large, which makes it difficult to obtain high performance.

Next, the conditional expression (2) defines a ratio of a focal length f1 of the first lens unit and the focal length ft at the telephoto end. When f1 and ft are in an appropriate relationship, a longitudinal chromatic aberration, which is problematic in a zoom lens that is usable up to the telephoto range, and a focus shift during zooming, which is problematic in a zoom lens that is usable in a telephoto range and has a high magnification, and is caused by a manufacturing error, may be suppressed.

When ft/f1 in the conditional expression (2) exceeds an upper limit, the focal length of the first lens unit becomes relatively too short with respect to the focal length at the telephoto end, and an enlargement magnification of the first lens unit on a telephoto side becomes too large. In the case where the enlargement magnification of the first lens unit is large, the longitudinal chromatic aberration generated in the first lens unit may no longer be corrected by the second and subsequent lens units, which makes it difficult to obtain high performance on the telephoto side. Further, a lateral magnification of the second lens unit becomes relatively large. In a case where various amounts of the second lens unit, here in particular a focal length, are shifted due to a manufacturing error of the second lens unit, the shift in focal length of the second lens unit also affects an image plane position. Now, when a lateral magnification of the second lens unit is represented by β2, a lateral magnification of the subsequent lens units is represented by βc, and an amount of shift in image position on the second lens unit itself is represented by Δsk2, a variation in imaging position, which is generated in the second lens unit, is enlarged to an amount of focus shift Δsk on an image plane in the following expression.

Δsk=Δsk2×(1−β2²)×βc ²  (x)

In regard to the expression (x), in the telephoto zoom lens having a high magnification as in the present invention, magnitudes of both β2 and βc become larger than 1 at the telephoto end. Therefore, when the lateral magnification of the second lens unit becomes relatively large, the manufacturing error of the second lens unit has a larger effect on the image plane position, with the result that the focus shift due to the zooming becomes difficult to suppress, which affects manufacturability.

When ft/f1 in the conditional expression (2) falls below a lower limit, the focal length of the first lens unit becomes too large, the first lens unit becomes difficult to downsize, and in addition, a spherical aberration and the longitudinal chromatic aberration, which are generated in the first lens unit, are increased and become difficult to correct by the other lens units.

Next, the conditional expression (3) defines a relationship of the focal length fw of the zoom lens at the wide angle end and the half angle of field ωw at the wide angle end with the focal length ft at the telephoto end. The denominator fw×tan ωw of the conditional expression (3) corresponds to a maximum image height at which the zoom lens may be used without a ray being eclipsed.

When ft/(fw×tan ωw) in the conditional expression (3) exceeds an upper limit, the focal length at the telephoto end becomes relatively too long. In this case, with a configuration in the conditional ranges defined by the above-mentioned conditional expressions, a focus movement due to the zooming cannot be suppressed, and further, the longitudinal chromatic aberration at the telephoto end also becomes difficult to correct. When ft/(fw×tan ωw) in the conditional expression (3) falls below a lower limit, with the configuration in the conditional ranges defined by the above conditions, the focal length of the first lens unit becomes relatively large, which makes it difficult to reduce the size and weight of the zoom lens.

It is preferred to set the numerical value ranges of the conditional expressions (1) to (3) as follows:

0.05<LN(|βct/|cw|)/LN(ft/fw)<0.40  (1a)

2.2<ft/f1<6.0  (2a)

25<ft/(fw×tan ωw)<115  (3a)

In each of the embodiments, it is more preferred to satisfy at least one of the following conditions.

The first lens unit includes a front lens unit having a positive refractive power, which includes at least one negative lens, and a rear lens unit having a negative refractive power, which includes one positive lens and one negative lens, and focal lengths of the lens units are represented by f1 f and f1 r, respectively. Moreover, a length from a surface vertex position of a lens surface closest to the object side to a surface vertex position of a lens surface closest to the image side of the first lens unit is represented by UD1. A lateral magnification of the second lens unit in the state in which focus is at infinity at the wide angle end is represented by β2 w. At this time, it is preferred to satisfy at least one of the following conditional expressions:

−0.50<f1f/f1r<−0.20  (4)

0.27<UD1/f1<0.55  (5)

−0.35<β2w<−0.15  (6)

The conditional expression (4) defines a relationship of the focal lengths of the front lens unit and the rear lens unit, which form the first lens unit. The front lens unit is configured to have a positive refractive power, the rear lens unit is configured to have a negative refractive power, and a configuration with which the conditional expression (4) is satisfied is adopted, with the result that weights of the first lens unit and the second and subsequent lens units that move during zooming may be reduced. FIGS. 14A and 14B are schematic diagrams illustrating paraxial relationships of the front lens unit and the rear lens unit. In FIGS. 14A and 14B, a ratio of the focal lengths of the sub lens units satisfies the following relationship:

f11a/f12a<f11b/f12b  (xi)

As illustrated in FIGS. 14A and 14B, a ray that is parallel to an optical axis enters from the image side of the first lens unit, and a position on the optical axis of a point at which the ray proceeds to the object side and intersects a ray that has passed through the rear lens unit and the front lens unit is an image side principal point position of the first lens unit. When the expression (xi) above is satisfied in FIGS. 14A and 14B, the focal length of the rear lens unit becomes relatively strong, with the result that an exit angle α′12 from the rear lens unit illustrated in FIGS. 14A and 14B becomes large, and an exit angle α′11 from the front lens unit becomes small. As a result, the image side principal point position, which is an intersection of the incident ray that is parallel to the optical axis and the exit ray from the front lens unit as illustrated in FIGS. 14A and 14B is displaced toward the object side. As a result of the principal point position being displaced toward the object side, an axial incident ray from the object side is subjected to a converging function more on the object side of the first lens unit, and a lens diameter of a sub lens unit on an exit side of the first lens unit, a diameter of the subsequent second lens unit, and a diameter of a lens barrel or the like holding the subsequent movable lens units may be reduced. In the case where a magnification is high and the focal length at the telephoto end is long as in the present invention, movement amounts of the movable lens units are large, and the lens diameters themselves tend to be very large, and hence the reductions in weight of the movable lens units lead to an improvement in portability, and also to simplification of functions required for driving the lenses.

When f1 f/f1 r in the conditional expression (4) exceeds an upper limit, the focal length of the rear lens unit becomes relatively too short, and the principal point of the first lens unit is significantly displaced toward the object side. As a result, a ray height of an off-axial ray that passes through a lens on the object side of the first lens unit is increased to increase the lens diameters, which makes the reductions in size and weight difficult. When f1 f/f1 r in the conditional expression (4) falls below a lower limit, the focal length of the rear lens unit becomes relatively too long, which makes it difficult to displace the principal point of the first lens unit toward the object side. As a result, the principal point of the first lens unit cannot be set to a desired value, and the reductions in size and weight become difficult.

The conditional expression (5) defines a relationship of a distance UD1 from a surface vertex closest to the object side to a surface vertex closest to the image side of the first lens unit and the focal length f1 of the first lens unit.

In a case where UD1/f1 in the conditional expression (5) exceeds an upper limit, a total thickness of the first lens unit becomes too large. The first lens unit is a lens unit having the largest lens diameter of the zoom lens, and when the first lens unit becomes large, the reductions in size and weight of the entire zoom lens become difficult. When UD1/f1 in the conditional expression (5) falls below a lower limit, the total thickness of the first lens unit becomes relatively too small. In this case, the refractive powers of the sub lens units forming the first lens unit become too strong, and amounts of aberrations generated in the sub lens units are increased, with the result that the longitudinal chromatic aberration, the spherical aberration, and coma become difficult to correct especially on the telephoto side.

The conditional expression (6) defines the lateral magnification β2 w of the second lens unit when focus is at infinity at the wide angle end.

When β2 w in the conditional expression (6) exceeds an upper limit, the lateral magnification of the second lens unit at the wide angle end becomes too large. In order to set the lateral magnification of the second lens unit large, there is a need to set a principal point interval between the first lens unit and the second lens unit large. Therefore, there is a need to make an air interval between the first lens unit and the second lens unit large, with the result that the total lens length becomes long, which makes it difficult to reduce the size and weight of the entire zoom lens. When β2 w in the conditional expression (6) falls below a lower limit, the movement amount during zooming becomes large on a wide angle side of the second lens unit, and the first lens unit and the second lens unit move away from a stop surface, with the result that the lens diameters of the first lens unit and the second lens unit increase, which makes it difficult to reduce the size and weight.

It is more preferred to set the numerical value ranges of the conditional expressions (4) to (6) as follows:

−0.47<f1f/f1r<−0.25  (4a)

0.29<UD1/f1<0.47  (5a)

−0.32<β2w<−0.19  (6a)

In another aspect of the zoom lens according to the present invention, it is preferred that lens units on the image side of the third lens unit include a fourth lens unit having a positive refractive power that moves during zooming, and a fifth lens unit having a positive refractive power that does not move for zooming. The fourth lens unit is added as a movable lens unit to increase flexibility in correcting the image plane during zooming so that a height of an off-axial incident ray on the first lens unit and ray heights of axial incident rays on the third and fourth lens units may be controlled, with the result that the lens units may be further downsized. Moreover, the fifth lens unit does not move for zooming so that an imaging relationship in the fifth lens unit becomes constant during zooming, with the result that a lens unit having an additional function, such as a vibration isolation unit, may be arranged in the fifth lens unit to simplify the control. In addition, even in a case where a focal length conversion unit such as an extender, which is retractably insertable on the optical axis, is provided in the fifth lens unit, such unit may be provided with a simple mechanism because there is no movable lens unit nearby.

In another aspect of the zoom lens according to the present invention, relative partial dispersions of optical materials to be used for the second lens unit are defined. In this case, the following conditional expression is satisfied:

−8.50×10⁻⁴<(θ2p−θ2n)/(ν2p−ν2n)<−2.00×10⁻⁴  (7)

where ν2 p and θ2 p represent average values of Abbe numbers and relative partial dispersions of convex lenses forming the second lens unit, respectively, and ν2 n and θ2 n represent average values of Abbe numbers and relative partial dispersions of concave lenses, respectively.

Here, the Abbe numbers and the relative partial dispersions of the materials of the optical device (lens) used in the present invention are defined as follows. Refractive indices with respect to a g-Line (435.8 nm), an F-Line (486.1 nm), a d-Line (587.6 nm), and a C-Line (656.3 nm) of Fraunhofer line are denoted by Ng, NF, Nd, and NC, respectively. The Abbe number νd and the relative partial dispersion θgF with respect to the g-Line and the F-Line are defined by the following expressions.

νd=(Nd−1)/(NF−NC)  (i)

θgF=(Ng−NF)/(NF−NC)  (ii)

The relative partial dispersion θgF of an existing optical material is present in a narrow range with respect to the Abbe number νd. Further, the existing optical material has a tendency that, as the Abbe number νd becomes smaller, the relative partial dispersion θgF becomes greater, that is, as the Abbe number νd becomes larger, the refractive index becomes lower. Here, a condition for correcting a chromatic aberration in a thin contact optical system including two lenses 1 and 2 having refractive powers φ1 and φ2 and Abbe numbers ν1 and ν2, respectively, is expressed by the following expression.

φ1/ν1+φ2/ν2=E  (iii)

In this case, a combined refractive power p of the lenses 1 and 2 is expressed by the following expression.

φ=φ1+φ2  (iv)

When E=0 is satisfied in expression (iii), in correcting the chromatic aberration, imaging positions of the C-Line and the F-Line match each other. At this time, φ1 and φ2 are expressed by the following expressions.

φ1=φ×ν1/(ν1−ν2)  (v)

φ2=φ×ν2/(ν1−ν2)  (vi)

FIG. 15 is a schematic diagram regarding two-color chromatic aberration correction and a remaining secondary spectrum of a lateral chromatic aberration of a lens unit LN having a negative refractive power and arranged between an object plane and an aperture stop. When the chromatic aberration of the negative lens unit LN illustrated in FIG. 15 is corrected, a material having a large Abbe number ν1 is used for a negative lens 1, and a material having a small Abbe number ν2 is used for a positive lens 2. Therefore, the negative lens 1 has a small relative partial dispersion 81 and the positive lens 2 has a large relative partial dispersion 82. When the lateral chromatic aberration is corrected for the C-Line and the F-Line, an imaging point of the g-Line shifts in a direction separated away from the optical axis. If an amount of the shift of the lateral chromatic aberration of the g-Line with respect to the C-Line and the F-Line is defined as a secondary spectrum amount ΔY, the secondary spectrum amount ΔY is expressed by the following expression.

ΔY=(1/φ)×(θ1−θ2)/(ν1−ν2)  (vii)

In order to satisfactorily correct the secondary spectrum of the lateral chromatic aberration over the entire zoom range, it is necessary to adjust an amount of the secondary spectrum of the lateral chromatic aberration generated in the second lens unit, which greatly affects the variations in the lateral chromatic aberration. The second lens unit has the negative refractive power. Hence, in order to satisfactorily correct the variation amount of the secondary spectrum of the lateral chromatic aberration over the entire zoom range, it is necessary to select such a glass material as to reduce the secondary spectrum amount ΔY generated in the second lens unit. The condition of the conditional expression (7) is defined so as to reduce an amount of the lateral chromatic aberration generated in the second lens unit. When the condition of an upper limit of the conditional expression (7) is not satisfied, a secondary spectrum of the lateral chromatic aberration is advantageously corrected, but refractive indices of concave lenses forming the second lens unit become low to reduce radii of curvature of the concave lenses. As a result, high order aberrations of a curvature of field and the coma increase, which makes it difficult to achieve good optical performance. When the condition of a lower limit of the conditional expression (7) is not satisfied, the secondary spectrum of the lateral chromatic aberration is increased, which makes it difficult to satisfactorily correct chromatic aberrations. It is more preferred to set the numerical value range of the conditional expression (7) as follows:

—7.70×10⁻⁴<(θ2p−θ2n)/(ν2p−ν2n)<−2.30×10⁻⁴  (7a)

In a further aspect of the zoom lens according to the present invention, relative partial dispersions of optical materials used in the first lens unit are defined. When average values of Abbe numbers and relative partial dispersions of convex lenses forming the first lens unit are represented by ν1 p and θ1 p, respectively, and average values of Abbe numbers and relative partial dispersions of concave lenses are represented by ν1 n and θ1 n, respectively, the following conditional expressions are satisfied:

−1.80×10⁻³<(θ1p−θ1n)/(ν1p−ν1n)<—0.80×10⁻³  (8)

FIG. 16 is a schematic diagram regarding two-color chromatic aberration correction of the longitudinal chromatic aberration by a positive lens unit PL and the remaining secondary spectrum. In FIG. 16, a material having a large Abbe number ν1 is used for a positive lens 1, and a material having a small Abbe number ν2 is used for a negative lens 2. Therefore, the positive lens 1 has a small relative partial dispersion 81, and the negative lens 2 has a large relative partial dispersion 82, with the result that when the longitudinal chromatic aberration is corrected by the C-Line and the F-Line, an imaging point of the g-Line is shifted toward the image side. When an amount of shift in the longitudinal chromatic aberration of the g-Line with respect to the C-Line and the F-Line in a case where a ray enters with an object distance being set to infinity is defined as an amount of secondary spectrum ΔS, the amount of secondary spectrum ΔS is expressed as:

ΔS=−(1/φ)×(θ1−θ2)/(ν1−ν2)  (xiii)

In order to satisfactorily correct a secondary spectrum of the longitudinal chromatic aberration at the telephoto end, there is a need to adjust a generation amount of the first lens unit in which the secondary spectrum is generated noticeably. As defined by the conditional expression (7), in an exemplary embodiment of the present invention, an optical material used in the second lens unit is devised so as to obtain a good secondary spectrum of the lateral chromatic aberration over the entire zoom range. As a result, in a case where an optical material used in the first lens unit does not include an appropriate material also, there arises a problem in that the longitudinal chromatic aberration is overcorrected especially at the telephoto end. The first lens unit has a positive refractive power, and in order to satisfactorily correct the secondary spectrum of the longitudinal chromatic aberration at the telephoto end, there is a need to determine the material so as to obtain an appropriate amount of correction of the amount of secondary spectrum ΔS generated in the first lens unit. The conditional expression (8) is defined so as to achieve the correction of the longitudinal chromatic aberration at the telephoto end and high optical performance. When the condition of an upper limit of the conditional expression (8) is not satisfied, the secondary spectrum of the longitudinal chromatic aberration at the telephoto end is advantageously corrected, but refractive indices of convex lenses forming the second lens unit are reduced, with the result that radii of curvature of the convex lenses forming the second lens unit become small. As a result, a high order aberration of the spherical aberration at the telephoto end is increased, which makes it difficult to achieve the good optical performance. When the condition of a lower limit of the conditional expression (8) is not satisfied, the secondary spectrum of the longitudinal chromatic aberration at the telephoto end is increased, which makes it difficult to satisfactorily correct chromatic aberrations at the telephoto end. It is more preferred to set the numerical value range of the conditional expression (8) as follows:

−1.60×10⁻³<(θ1p−1n)/(ν1p−ν1n)<−1.00×10⁻³  (8a)

A specific configuration of the zoom lens of the present invention is described below by way of features of lens configurations of Embodiments 1 to 6 and Numerical Embodiments 1 to 6 corresponding thereto, respectively.

Embodiment 1

FIG. 1 is a lens cross-sectional view when focus is at an object at infinity at the wide angle end (short focal length end) in Numerical Embodiment 1 as Embodiment 1 of the present invention. FIGS. 2A, 2B, and 2C are aberration diagrams when focus is at infinity at the wide angle end, when focus is at infinity at a zoom position having a focal length of 200 mm, and when focus is at infinity at the telephoto end, respectively. In the lens cross-sectional views, the left side is a subject (object) side (front side), and the right side is the image side (rear side). A first lens unit U1 having a positive refractive power that does not move includes, in order from the object side to the image side, a first sub lens unit U11 having a positive refractive power, a second sub lens unit U12 having a positive refractive power, and a third sub lens unit U13 having a negative refractive power. A second lens unit U2 having the negative refractive power that moves during zooming is moved on the optical axis toward the image plane side to perform zooming from the wide angle end to the telephoto end. A third lens unit U3 having a positive refractive power and a fourth lens unit U4 having a positive refractive power both move on the optical axis during zooming from the wide angle end to the telephoto end. An aperture stop SP does not move in an optical axis direction, and a fifth lens unit (relay lens unit) U5 having a positive refractive power that does not move has an imaging function. In the fifth lens unit U5, a converter (extender) for converting the focal length or the like may be mounted. An image plane IP corresponds to the imaging surface such as a solid-state image pickup element or a film surface. The focusing may be performed by moving a part of the first lens unit, such as the sub lens unit U12, in the optical axis direction, or by moving the second lens unit and the subsequent movable lens units or a part of fixed lens units.

In the aberration diagrams, the straight line, the broken line, the one-dot chain line, and the two-dot chain line in the spherical aberration represent an e-Line, the F-Line, the C-Line, and the g-Line, respectively. The solid line and the one-dot chain line in astigmatism represent a sagittal image plane (ΔS) and a meridional image plane (ΔM), respectively, and the broken line, the one-dot chain line, and the two-dot chain line in the lateral chromatic aberration represent the F-Line, the C-Line, and the g-Line, respectively. The astigmatism and the lateral chromatic aberration are illustrated as amounts of aberrations when a ray that passes through a center of a light flux at a stop position is assumed to be a principal ray. A paraxial half angle of field is represented by w, and an F-number is denoted by Fno. In longitudinal aberration diagrams, the spherical aberration, the astigmatism, a distortion, and the lateral chromatic aberration are drawn at scales of 0.5 mm, 0.5 mm, 5%, and 0.05 mm, respectively. Note that, in the following embodiments, the terms “wide angle end” and “telephoto end” refer to zoom positions at times when the second lens unit is located at both ends of a range in which the second lens unit is mechanically movable on the optical axis, respectively. The above descriptions on the lens cross-sectional views and the aberration diagrams are the same also in the following embodiments unless otherwise specified.

The first to fourth lens units in Numerical Embodiment 1 as Embodiment 1 are described. In Numerical Embodiment 1, the first lens unit U1 corresponds to the first to fourteenth lens surfaces, and includes, in order from the object side to the image side, the first sub lens unit having a positive refractive power, the second sub lens unit having a positive refractive power, and a third sub lens unit having a negative refractive power. The first sub lens unit having the positive refractive power includes, in order from the object side to the image side, two positive lenses and a negative lens. The second sub lens unit having the positive refractive power includes, in order from the object side to the image side, a positive lens, and a cemented positive lens formed by cementing a positive lens and a negative lens, and the second sub lens unit is moved in the optical axis direction to perform focus adjustment. The third sub lens unit includes a cemented negative lens formed by cementing a positive lens and a negative lens. The second lens unit U2 corresponds to the fifteenth to twenty-fifth lens surfaces in Numerical Embodiment 1, and includes, in order from the object side to the image side, a negative lens, a cemented negative lens formed by cementing a positive lens and a negative lens, a negative lens, a positive lens, and a negative lens. The third lens unit U3 corresponds to the twenty-sixth to thirty-first lens surfaces in Numerical Embodiment 1, and includes, in order from the object side to the image side, a positive lens, a negative lens, and a positive lens. The fourth lens unit U4 corresponds to the thirty-second to thirty-seventh lens surfaces in Numerical Embodiment 1, and includes, in order from the object side to the image side, a positive lens, a negative lens, and a positive lens. An aspherical surface is used for the twenty-ninth surface to correct variations in coma and spherical aberration due to zooming. Note that, in this embodiment, the front lens unit corresponds to the first and second sub lens units and f1 f corresponds to a combined focal length of the first and second sub lens units in the state in which focus is at infinity, and the rear lens unit corresponds to the third sub lens unit and f1 r corresponds to a focal length of the third sub lens unit.

Table 1 shows values corresponding to the conditional expressions in Embodiment 1. In this numerical embodiment, all of the conditional expressions are satisfied to achieve the good optical performance. In addition, the zoom lens, which is usable in the super telephoto range and has the high magnification and a large aperture, has a focal length at the wide angle end of 50 mm, a magnification of 20×, a large maximum image height of 15.55 mm, an F-number at the wide angle end of 4.5, and an F-number at the telephoto end of 7.4, and achieves the reduction in size at the same time.

Embodiment 2

First to fourth lens units in Numerical Embodiment 2 as Embodiment 2 are described. In Numerical Embodiment 2, the first lens unit U1 corresponds to the first to thirteenth lens surfaces, and includes, in order from the object side to the image side, the first sub lens unit having a positive refractive power and the second sub lens unit having a negative refractive power. The first sub lens unit having the positive refractive power includes, in order from the object side to the image side, two positive lenses, a negative lens, and two positive lenses. The second sub lens unit includes a cemented negative lens formed by cementing a positive lens and a negative lens, and the second sub lens unit is moved in the optical axis direction to perform focus adjustment. The second lens unit U2 corresponds to the fourteenth to twenty-third lens surfaces in Numerical Embodiment 2, and includes, in order from the object side to the image side, a cemented negative lens formed by cementing a positive lens and a negative lens, a negative lens, a cemented positive lens formed by cementing a positive lens and a negative lens, and a negative lens. The third lens unit U3 corresponds to the twenty-fourth to twenty-eighth lens surfaces in Numerical Embodiment 2, and includes, in order from the object side to the image side, a cemented positive lens formed by cementing a positive lens and a negative lens, and a positive lens. The fourth lens unit U4 corresponds to the twenty-ninth to thirty-third lens surfaces in Numerical Embodiment 2, and includes, in order from the object side to the image side, a positive lens, and a cemented lens formed by cementing a negative lens and a positive lens. Aspherical surfaces are used for the twenty-seventh surface and the twenty-eighth surface to correct the variations in coma and spherical aberration due to the zooming. Note that, in this embodiment, the front lens unit corresponds to the first and second sub lens units and f1 f corresponds to a combined focal length of the first and second sub lens units in the state in which focus is at infinity, and the rear lens unit corresponds to the third sub lens unit and f1 r corresponds to a focal length of the third sub lens unit.

Table 1 shows values corresponding to the conditional expressions in Embodiment 2. In this numerical embodiment, all of the conditional expressions are satisfied to achieve the good optical performance. In addition, the zoom lens, which is usable in the super telephoto range and has the high magnification and a large aperture, has a focal length at the wide angle end of 60 mm, a magnification of 15×, a large maximum image height of 15.55 mm, an F-number at the wide angle end of 4.5, and an F-number at the telephoto end of 7.0, and achieves the reduction in size at the same time.

Embodiment 3

First to fourth lens units in Numerical Embodiment 3 as Embodiment 3 are described. In Numerical Embodiment 3, the first lens unit U1 corresponds to the first to fourteenth lens surfaces, and includes, in order from the object side to the image side, the first sub lens unit having a positive refractive power, the second sub lens unit having a positive refractive power, and a third sub lens unit having a negative refractive power. The first sub lens unit having the positive refractive power includes, in order from the object side to the image side, two positive lenses and a negative lens. The second sub lens unit having the positive refractive power includes, in order from the object side to the image side, a positive lens, and a cemented positive lens formed by cementing a positive lens and a negative lens, and the second sub lens unit is moved in the optical axis direction to perform focus adjustment. The third sub lens unit includes a cemented negative lens formed by cementing a positive lens and a negative lens. The second lens unit U2 corresponds to the fifteenth to twenty-fifth lens surfaces in Numerical Embodiment 3, and includes, in order from the object side to the image side, two negative lenses, a cemented negative lens formed by cementing a positive lens and a negative lens, a positive lens, and a negative lens. The third lens unit U3 corresponds to the twenty-sixth to thirty-first lens surfaces in Numerical Embodiment 3, and includes, in order from the object side to the image side, a positive lens, a negative lens, and a positive lens. The fourth lens unit U4 corresponds to the thirty-second to thirty-sixth lens surfaces in Numerical Embodiment 3, and includes, in order from the object side to the image side, a positive lens and a cemented lens formed by cementing a negative lens and a positive lens. An aspherical surface is used for the twenty-ninth surface to correct variations in coma and spherical aberration due to zooming. Note that, in this embodiment, the front lens unit corresponds to the first and second sub lens units and f1 f corresponds to a combined focal length of the first and second sub lens units in the state in which focus is at infinity, and the rear lens unit corresponds to the third sub lens unit and f1 r corresponds to a focal length of the third sub lens unit.

Table 1 shows values corresponding to the conditional expressions in Embodiment 3. In this numerical embodiment, all of the conditional expressions are satisfied to achieve the good optical performance. In addition, the zoom lens, which is usable in the super telephoto range and has the high magnification and a large aperture, has a focal length at the wide angle end of 50 mm, a magnification of 10×, a large maximum image height of 15.55 mm, an F-number at the wide angle end of 4.0, and an F-number at the telephoto end of 5.0, and achieves the reduction in size at the same time.

Embodiment 4

First to fourth lens units in Numerical Embodiment 4 as Embodiment 4 are described. In Numerical Embodiment 4, the first lens unit U1 corresponds to the first to fourteenth lens surfaces, and includes, in order from the object side to the image side, the first sub lens unit having a positive refractive power, the second sub lens unit having a positive refractive power, and a third sub lens unit having a negative refractive power. The first sub lens unit having the positive refractive power includes, in order from the object side to the image side, two positive lenses and a negative lens. The second sub lens unit having the positive refractive power includes, in order from the object side to the image side, a positive lens, and a cemented positive lens formed by cementing a positive lens and a negative lens, and the second sub lens unit is moved in the optical axis direction to perform focus adjustment. The third sub lens unit includes a cemented negative lens formed by cementing a positive lens and a negative lens. The second lens unit U2 corresponds to the fifteenth to twenty-fifth lens surfaces in Numerical Embodiment 4, and includes, in order from the object side to the image side, two negative lenses, a cemented negative lens formed by cementing a positive lens and a negative lens, a positive lens, and a negative lens. The third lens unit U3 corresponds to the twenty-sixth to thirty-first lens surfaces in Numerical Embodiment 4, and includes, in order from the object side to the image side, a positive lens, a negative lens, and a positive lens. The fourth lens unit U4 corresponds to the thirty-second to thirty-seventh lens surfaces in Numerical Embodiment 4, and includes, in order from the object side to the image side, a positive lens, a negative lens, and a positive lens. Aspherical surfaces are used for the fifteenth, twenty-second, twenty-ninth, and forty-ninth surfaces to suppress a variation in off-axial aberration by the fifteenth and twenty-second surfaces, the variations in spherical aberration and coma by the twenty-ninth surface, and a high-order image plane aberration in a high image height by the forty-ninth surface. Note that, in this embodiment, the front lens unit corresponds to the first and second sub lens units and f1 f corresponds to a combined focal length of the first and second sub lens units in the state in which focus is at infinity and the rear lens unit corresponds to the third sub lens units and f1 r corresponds to a focal length of the third sub lens unit.

Table 1 shows values corresponding to the conditional expressions in Embodiment 4. In this numerical embodiment, all of the conditional expressions are satisfied to achieve the good optical performance. In addition, the zoom lens, which is usable in the super telephoto range and has the high magnification and a large aperture, has a focal length at the wide angle end of 50 mm, a magnification of 20×, a large maximum image height of 21.64 mm, an F-number at the wide angle end of 4.5, and an F-number at the telephoto end of 7.5, and achieves the reduction in size at the same time.

Embodiment 5

First to fourth lens units in Numerical Embodiment 5 as Embodiment 5 are described. In Numerical Embodiment 5, the first lens unit U1 corresponds to the first to fourteenth lens surfaces, and includes, in order from the object side to the image side, the first sub lens unit having a positive refractive power, the second sub lens unit having a positive refractive power, and a third sub lens unit having a negative refractive power. The first sub lens unit having the positive refractive power includes, in order from the object side to the image side, two positive lenses and a negative lens. The second sub lens unit having the positive refractive power includes, in order from the object side to the image side, a positive lens, and a cemented positive lens formed by cementing a positive lens and a negative lens, and the second sub lens unit is moved in the optical axis direction to perform focus adjustment. The third sub lens unit includes a cemented negative lens formed by cementing a positive lens and a negative lens. The second lens unit U2 corresponds to the fifteenth to twenty-fourth lens surfaces in Numerical Embodiment 5, and includes, in order from the object side to the image side, a negative lens, a cemented negative lens formed by cementing a negative lens and a positive lens, a cemented negative lens formed by cementing a negative lens and a positive lens, and a negative lens. The third lens unit U3 corresponds to the twenty-fifth to thirtieth lens surfaces in Numerical Embodiment 5, and includes, in order from the object side to the image side, a positive lens, a negative lens, and a positive lens. The fourth lens unit U4 corresponds to the thirty-first to thirty-fifth lens surfaces in Numerical Embodiment 5, and includes, in order from the object side to the image side, a positive lens, a negative lens, and a positive lens. Aspherical surfaces are used for the fifteenth, twenty-eighth, thirty-first, and forty-second surfaces to suppress a variation in off-axial aberration by the fifteenth surface, the variations in spherical aberration and coma by the twenty-eighth and thirty-first surfaces, and a high-order image plane aberration in a high image height by the forty-second surface. Note that, in this embodiment, the front lens unit corresponds to the first and second sub lens units and f1 f corresponds to a combined focal length of the first and second sub lens units in the state in which focus is at infinity, and the rear lens unit corresponds to the third sub lens unit and f1 r corresponds to a focal length of the third sub lens unit.

Table 1 shows values corresponding to the conditional expressions in Embodiment 5. In this numerical embodiment, all of the conditional expressions are satisfied to achieve the good optical performance. In addition, the zoom lens, which is usable in the super telephoto range and has the high magnification and a large aperture, has a focal length at the wide angle end of 50 mm, a magnification of 30×, a large maximum image height of 14.0 mm, an F-number at the wide angle end of 4.5, and an F-number at the telephoto end of 10.0, and achieves the reduction in size at the same time.

Embodiment 63

First to fourth lens units in Numerical Embodiment 6 as Embodiment 6 are described. The first lens unit U1 corresponds to the first to twelfth lens surfaces in Numerical Embodiment 6, and includes, in order from the object side to the image side, a first sub lens unit having a very weak negative refractive power, and a second sub lens unit having a positive refractive power. The first sub lens unit having the negative refractive power includes, in order from the object side to the image side, a negative lens, a positive lens, a negative lens, and a positive lens. The second sub lens unit having the positive refractive power includes, in order from the object side to the image side, two positive lenses, and moves the second sub lens unit in the optical axis direction to perform the focus adjustment. The second lens unit U2 corresponds to the thirteenth to twenty-third lens surfaces in Numerical Embodiment 6, and includes, in order from the object side to the image side, two negative lenses, a cemented positive lens formed by cementing a positive lens and a negative lens, a negative lens, and a positive lens. The third lens unit U3 corresponds to the twenty-fourth to twenty-ninth lens surfaces in Numerical Embodiment 6, and includes, in order from the object side to the image side, a positive lens, a negative lens, and a positive lens. The fourth lens unit U4 corresponds to the thirtieth to thirty-fifth lens surfaces in Numerical Embodiment 6, and includes, in order from the object side to the image side, a positive lens, a negative lens, and a positive lens. An aspherical surface is used for the twenty-seventh surface to suppress variations in spherical aberration and coma. Note that, in this embodiment, the front lens unit corresponds to the first sub lens unit and f1 f corresponds to a focal length of the first sub lens unit, and the rear lens unit corresponds to the second sub lens unit and f1 r corresponds to a focal length of the second sub lens unit.

Table 1 shows values corresponding to the conditional expressions in Embodiment 6. In this numerical embodiment, the conditional expressions (1) to (3) and (5) to (8) are satisfied to achieve the good optical performance. In addition, the zoom lens, which is usable in the super telephoto range and has the high magnification and a large aperture, has a focal length at the wide angle end of 40 mm, a magnification of 20×, a large maximum image height of 15.55 mm, an F-number at the wide angle end of 4.5, and an F-number at the telephoto end of 5.6, and achieves the reduction in size at the same time.

NUMERICAL EMBODIMENTS

Next, Numerical Embodiments 1 to 6 corresponding to Embodiments 1 to 6 of the present invention are shown below. In each of the numerical embodiments, symbol “i” represents the order of a surface from the object side, symbol “ri” represents a radius of curvature of an i-th surface from the object side, symbol “di” represents an interval between the i-th surface and an (i+1)th surface from the object side, and symbols “ndi” and “νdi” respectively represent a refractive index and an Abbe number of an optical material between the i-th surface and the (i+1)th surface. The focal length, the F-number, and the angle of field represent values when focus is at infinity. Symbol BF is an air conversion value of a distance from the final surface of the lens to the image plane.

Note that, the aspherical shape is expressed by the following expression:

x=(y ² /r)/{1+(1−k×y ² /r ²)^(0.5) }+A4×y ⁴ +A6×y ⁶ +A8×y ⁸ +A10×y ¹⁰ A12×y ¹²

where x represents a coordinate in the optical axis direction, y represents a coordinate in a direction perpendicular to the optical axis, r represents a reference radius of curvature, k represents a conic constant, and An represents an n-th order aspherical coefficient, provided that “e−x” means “×10 ^(−x)”. Note that, the lens surfaces having the aspherical surfaces are marked with asterisks (*) on the left side of surface numbers in the tables.

Table 1 shows the correspondence between each of the embodiments and each of the above-mentioned conditional expressions.

Numerical Embodiment 1

Surface Effective Focal number r d nd νd θgF diameter length 1 246.68132 17.57134 1.433870 95.10 0.5373 137.561 379.844 2 −489.49126 0.70000 1.000000 0.00 0.0000 136.362 0.000 3 251.80653 14.77425 1.433870 95.10 0.5373 130.301 419.328 4 −649.85945 1.00394 1.000000 0.00 0.0000 128.957 0.000 5 −509.36354 4.00000 1.720467 34.70 0.5834 128.865 −393.778 6 652.48261 14.44601 1.000000 0.00 0.0000 125.445 0.000 7 255.23550 10.29049 1.433870 95.10 0.5373 118.241 558.103 8 −4902.84082 0.20000 1.000000 0.00 0.0000 117.027 0.000 9 197.35639 12.59513 1.438750 94.93 0.5343 111.945 420.679 10 −2906.58993 2.50000 1.720467 34.70 0.5834 109.606 −882.774 11 821.58629 2.94687 1.000000 0.00 0.0000 107.326 0.000 12 1913.20539 6.71999 1.761821 26.52 0.6135 105.877 536.079 13 −524.31136 2.20000 1.618000 63.33 0.5441 104.412 −267.162 14 242.71285 (Variable) 1.000000 0.00 0.0000 99.476 0.000 15 −860.74296 1.80000 1.816000 46.62 0.5568 50.656 −89.348 16 80.17496 3.81547 1.000000 0.00 0.0000 47.151 0.000 17 375.28281 7.31173 1.720467 34.70 0.5834 46.543 69.386 18 −57.65105 1.50000 1.595220 67.74 0.5442 45.806 −66.490 19 128.90141 4.07926 1.000000 0.00 0.0000 41.685 0.000 20 −92.43936 1.50000 1.595220 67.74 0.5442 41.683 −65.212 21 67.72717 0.10000 1.000000 0.00 0.0000 40.314 0.000 22 55.67072 6.08760 1.720467 34.70 0.5834 40.359 67.855 23 −405.29323 2.13101 1.000000 0.00 0.0000 39.833 0.000 24 −77.78064 1.40000 1.595220 67.74 0.5442 39.815 −74.269 25 103.94566 (Variable) 1.000000 0.00 0.0000 38.960 0.000 26 116.76899 6.42003 1.618000 63.33 0.5441 43.512 79.194 27 −83.01992 0.02878 1.000000 0.00 0.0000 43.578 0.000 28 −86.18403 1.50000 1.834000 37.16 0.5775 43.539 −92.667 *29 803.67833 0.20000 1.000000 0.00 0.0000 43.982 0.000 30 120.27059 5.59541 1.496999 81.54 0.5374 44.453 130.541 31 −139.57348 (Variable) 1.000000 0.00 0.0000 44.522 0.000 32 87.58614 4.42301 1.487490 70.23 0.5300 43.877 183.090 33 3911.73924 0.20000 1.000000 0.00 0.0000 43.479 0.000 34 86.15302 1.50000 1.720457 34.70 0.5834 42.506 −168.527 35 50.16723 1.21338 1.000000 0.00 0.0000 41.157 0.000 36 66.35327 5.30796 1.496999 81.54 0.5374 41.151 116.995 37 −468.67849 (Variable) 1.000000 0.00 0.0000 40.725 0.000 38 (Stop) 0.00000 10.51965 1.000000 0.00 0.0000 28.657 0.000 39 603.24912 1.40000 1.882997 40.76 0.5667 23.839 −48.954 40 40.51116 0.15000 1.000000 0.00 0.0000 23.084 0.000 41 35.62346 4.10373 1.805181 25.42 0.6161 23.101 36.637 42 −171.92350 3.92591 1.000000 0.00 0.0000 22.594 0.000 43 −109.90676 1.50000 1.910820 35.25 0.5824 20.117 −33.390 44 42.71602 33.00000 1.000000 0.00 0.0000 19.407 0.000 45 90.18955 6.39772 1.496999 81.54 0.5374 30.314 68.285 46 −53.37817 5.55492 1.000000 0.00 0.0000 30.620 0.000 47 −138.46821 4.00000 1.882997 40.76 0.5667 29.643 −36.072 48 42.24648 5.86644 1.603420 38.03 0.5835 29.852 66.251 49 −797.00609 0.15000 1.000000 0.00 0.0000 30.355 0.000 50 114.93981 7.37952 1.517417 52.43 0.5564 30.683 53.618 51 −35.98055 3.00000 1.882997 40.76 0.5667 30.879 −98.457 52 −63.53396 (BF) 1.000000 0.00 0.0000 31.927 0.000 Image plane ∞ Aspherical surface data Twenty-ninth surface K = 9.77619e+002 A4 = 1.75645e−007 A6 = −1.54674e−011 A8 = −1.21139e−012 A10 = 2.79900e−015 A12 = −3.45030e−018 Various data Zoom ratio 20.00 Wide angle Intermediate Telephoto Focal length 50.00 200.00 1000.00 F number 4.50 4.50 7.40 Half angle of field 17.28 4.45 0.89 Image height 15.55 15.55 15.55 Total lens length 493.74 493.74 493.74 BF 66.76 66.76 66.76 d14 5.00 84.76 132.18 d25 162.25 77.28 3.00 d31 24.90 9.14 40.88 d37 1.82 22.78 17.91 Zoom lens unit data Unit First surface Focal length 1 1 255.00 2 15 −34.75 3 26 105.00 4 32 125.00 5 38 −605.15

Numerical Embodiment 2

Surface Effective Focal number r d nd νd θgF diameter length 1 270.17928 15.13046 1.433870 95.10 0.5373 130.169 407.710 2 −507.30992 0.20171 1.000000 0.00 0.0000 129.580 0.000 3 195.46941 13.65616 1.433870 95.10 0.5373 124.249 481.146 4 2899.45736 9.30808 1.000000 0.00 0.0000 122.342 0.000 5 −479.70303 3.00000 1.800000 29.84 0.6017 119.105 −388.923 6 908.20312 0.96409 1.000000 0.00 0.0000 117.139 0.000 7 295.93269 11.79869 1.433870 95.10 0.5373 115.660 440.626 8 −537.32876 1.45510 1.000000 0.00 0.0000 114.642 0.000 9 158.77485 11.37494 1.433870 95.10 0.5373 106.811 465.192 10 721.42143 2.11266 1.000000 0.00 0.0000 104.386 0.000 11 774.60480 7.65730 1.800000 29.84 0.6017 102.789 316.577 12 −379.05422 2.20000 1.743198 49.34 0.5530 101.523 −170.137 13 191.59077 (Variable) 1.000000 0.00 0.0000 95.371 0.000 14 306.46548 6.29897 1.720467 34.70 0.5834 46.492 98.717 15 −92.63364 1.80000 1.772499 49.60 0.5521 44.594 −41.170 16 49.20051 6.82093 1.000000 0.00 0.0000 38.932 0.000 17 −97.47695 1.50000 1.595220 67.74 0.5442 38.473 −82.245 18 99.61135 0.15000 1.000000 0.00 0.0000 37.660 0.000 19 69.28990 5.66183 1.800000 29.84 0.6017 37.640 59.953 20 −154.06464 1.00000 1.496999 81.54 0.5374 37.136 −175.321 21 202.36374 3.49735 1.000000 0.00 0.0000 36.056 0.000 22 −62.48999 1.40000 1.595220 67.74 0.5442 36.038 −82.553 23 235.75049 (Variable) 1.000000 0.00 0.0000 35.802 0.000 24 108.87034 6.22491 1.595220 67.74 0.5442 41.732 78.622 25 −80.81998 1.50000 1.834000 37.16 0.5775 41.823 −94.228 26 3721.87578 0.20000 1.000000 0.00 0.0000 42.359 0.000 *27 204.87400 4.21540 1.583126 59.38 0.5423 42.639 143.950 *28 −142.08754 (Variable) 1.000000 0.00 0.0000 42.768 0.000 29 210.29170 4.22394 1.487490 70.23 0.5300 42.592 176.200 30 −145.08052 0.20000 1.000000 0.00 0.0000 42.449 0.000 31 74.94026 1.50000 1.720467 34.70 0.5834 41.129 −126.894 32 40.96106 7.05734 1.496999 81.54 0.5374 39.624 84.510 33 1398.05586 (Variable) 1.000000 0.00 0.0000 38.991 0.000 34 (Stop) 0.00000 10.53028 1.000000 0.00 0.0000 28.093 0.000 35 126.06891 1.40000 1.882997 40.76 0.5667 23.147 −62.020 36 38.13355 0.15000 1.000000 0.00 0.0000 22.330 0.000 37 28.91783 4.11703 1.805181 25.42 0.6161 22.279 35.238 38 −2749.18415 1.09107 1.000000 0.00 0.0000 21.525 0.000 39 −286.78566 1.50000 1.910820 35.25 0.5824 20.805 −28.586 40 28.92117 33.00000 1.000000 0.00 0.0000 19.622 0.000 41 70.74415 6.88294 1.496999 81.54 0.5374 30.454 62.449 42 −53.78764 5.53775 1.000000 0.00 0.0000 30.680 0.000 43 −109.72301 4.00000 1.882997 40.76 0.5667 29.415 −35.634 44 45.23886 8.00963 1.603420 38.03 0.5835 29.636 39.386 45 −47.34010 0.15000 1.000000 0.00 0.0000 30.120 0.000 46 −115.77129 5.47766 1.501372 56.42 0.5533 29.869 93.498 47 −33.99699 3.00000 1.882997 40.76 0.5667 29.828 −68.273 48 −80.59641 (BF) 1.000000 0.00 0.0000 30.746 0.000 Image plane ∞ Aspherical surface data Twenty-seventh surface K = 1.58925e+001 A4 = −7.43425e−007 A6 = 1.04684e−010 A8 = 2.14168e−013 A10 = −8.73048e−016 A12 = 1.85388e−018 Twenty-eighth surface K = −1.09433e+001 A4 = −3.39181e−007 A6 = 3.00641e−010 A8 = −2.80726e−013 A10 = 1.32329e−016 A12 = 1.13931e−018 Various data Zoom ratio 15.00 Wide angle Intermediate Telephoto Focal length 60.00 240.00 900.00 F number 4.50 4.50 7.00 Half angle of field 14.53 3.71 0.99 Image height 15.55 15.55 15.55 Total lens length 458.15 458.15 458.15 BF 65.00 65.00 65.00 d13 17.12 86.73 128.82 d23 130.97 57.75 1.67 d28 25.40 8.04 37.61 d33 2.70 23.67 8.09 Zoom lens unit data Unit First surface Focal length 1 1 245.59 2 14 −34.00 3 24 110.00 4 29 105.00 5 34 −361.71

Numerical Embodiment 3

Surface Effective Focal number r d nd νd θgF diameter length 1 14683.19138 4.28544 1.487490 70.23 0.5300 100.000 1721.757 2 −893.35269 0.70000 1.000000 0.00 0.0000 99.993 0.000 3 362.01860 11.51442 1.433870 95.10 0.5373 99.670 332.370 4 −238.35968 0.35944 1.000000 0.00 0.0000 99.317 0.000 5 −231.46543 2.50000 2.001000 29.13 0.5997 99.238 −427.694 6 −501.88128 8.57177 1.000000 0.00 0.0000 99.455 0.000 7 240.55692 10.07997 1.433870 95.10 0.5373 97.514 364.940 8 −460.74683 0.20000 1.000000 0.00 0.0000 96.985 0.000 9 144.71298 12.03462 1.438750 94.93 0.5343 92.816 263.769 10 −570.27449 2.40000 1.834000 37.16 0.5775 91.583 −769.155 11 −4898.86844 1.00000 1.000000 0.00 0.0000 90.227 0.000 12 619.25437 7.09837 1.800000 29.84 0.6017 88.390 265.204 13 −324.96638 2.30000 1.772499 49.60 0.5521 87.309 −178.464 14 242.19484 (Variable) 1.000000 0.00 0.0000 83.470 0.000 15 −178.55461 1.20000 1.816000 46.62 0.5568 37.386 −47.096 16 49.43883 5.59373 1.000000 0.00 0.0000 35.028 0.000 17 −71.20411 1.20000 1.496999 81.54 0.5374 34.990 −117.033 18 324.58556 0.10000 1.000000 0.00 0.0000 35.168 0.000 19 107.25329 6.59981 1.720467 34.70 0.5834 35.303 44.268 20 −44.64885 1.20000 1.496999 81.54 0.5374 35.198 −58.246 21 83.75158 0.10000 1.000000 0.00 0.0000 33.794 0.000 22 55.75224 2.24505 1.720467 34.70 0.5834 33.679 264.958 23 77.20356 3.84124 1.000000 0.00 0.0000 33.200 0.000 24 −75.98380 1.20000 1.496999 81.54 0.5374 33.148 −145.873 25 1696.98389 (Variable) 1.000000 0.00 0.0000 33.097 0.000 26 10721.79237 4.47902 1.516330 64.14 0.5352 38.162 122.892 27 −64.06026 0.20000 1.000000 0.00 0.0000 38.506 0.000 28 −66.50266 1.00000 1.720467 34.70 0.5834 38.514 −107.550 *29 −453.51248 0.20000 1.000000 0.00 0.0000 39.451 0.000 30 102.12806 6.96953 1.438750 94.93 0.5343 40.558 98.351 31 −73.48540 (Variable) 1.000000 0.00 0.0000 40.893 0.000 32 75.33389 5.78775 1.438750 94.93 0.5343 40.711 126.948 33 −210.70991 0.20000 1.000000 0.00 0.0000 40.346 0.000 34 56.18515 1.00000 1.720467 34.70 0.5834 32.729 −92.170 35 30.30107 7.72184 1.516330 64.14 0.5352 36.804 63.732 36 334.95037 (Variable) 1.000000 0.00 0.0000 36.043 0.000 37 (Stop) 0.00000 3.42568 1.000000 0.00 0.0000 27.363 0.000 38 −76.00199 1.00000 1.882997 40.76 0.5667 26.135 −44.367 39 82.33763 4.78571 1.728250 28.46 0.6077 25.808 45.929 40 −55.71617 1.50000 1.000000 0.00 0.0000 25.614 0.000 41 −381.14533 1.00000 1.834807 42.73 0.5648 24.140 −108.480 42 119.79483 0.50000 1.000000 0.00 0.0000 23.697 0.000 43 20.43624 3.50000 1.717362 29.50 0.6048 22.717 86.590 44 28.15792 1.69497 1.000000 0.00 0.0000 21.225 0.000 45 84.59384 1.00000 1.882997 40.76 0.5667 21.053 −53.858 46 30.38613 35.00000 1.000000 0.00 0.0000 20.141 0.000 47 −36.11799 4.82364 1.438750 94.93 0.5343 24.588 73.242 48 −17.72245 1.00000 1.834807 42.73 0.5648 25.142 −49.165 49 −31.85952 0.50000 1.000000 0.00 0.0000 27.172 0.000 50 65.20672 1.00000 1.834807 42.73 0.5648 29.231 −55.093 51 26.86796 6.87418 1.517417 52.43 0.5564 29.218 43.868 52 −137.45767 0.50000 1.000000 0.00 0.0000 29.715 0.000 53 28.89595 3.99950 1.516330 64.14 0.5352 31.634 138.643 54 46.05030 (BF) 1.000000 0.00 0.0000 31.149 0.000 Image plane ∞ Aspherical surface data Twenty-ninth surface K = 1.99297e+002 A4 = 8.40121e−007 A6 = 5.66873e−010 A8 = −1.71055e−012 A10 = 4.35647e−015 A12 = −3.59753e−018 Various data Zoom ratio 10.00 Wide angle Intermediate Telephoto Focal length 50.00 200.00 500.00 F number 4.00 4.00 5.00 Half angle of field 17.28 4.45 1.78 Image height 15.55 15.55 15.55 Total lens length 376.01 376.01 376.01 BF 44.09 44.09 44.09 d14 3.45 85.24 113.85 d25 100.00 38.45 1.59 d31 40.00 5.99 13.31 d36 2.49 16.26 17.19 Zoom lens unit data Unit First surface Focal length 1 1 205.00 2 15 −34.50 3 26 110.50 4 32 80.00 5 37 −159.71

Numerical Embodiment 4

Surface Effective Focal number r d nd νd θgF diameter length 1 326.67857 15.75842 1.433870 95.10 0.5373 140.491 444.392 2 −466.47547 0.70000 1.000000 0.00 0.0000 139.266 0.000 3 230.77526 14.96465 1.433870 95.10 0.5373 129.287 400.768 4 −698.54118 1.00000 1.000000 0.00 0.0000 128.099 0.000 5 −508.72076 4.00000 1.720467 34.70 0.5834 128.179 −337.657 6 473.91513 7.39981 1.000000 0.00 0.0000 124.692 0.000 7 524.01780 9.36516 1.433870 95.10 0.5373 122.616 661.210 8 −634.00814 0.15000 1.000000 0.00 0.0000 121.818 0.000 9 141.42849 15.45709 1.438750 94.93 0.5343 114.688 304.168 10 −2394.32576 2.50000 1.720467 34.70 0.5834 113.156 −1081.591 11 1167.46931 1.21229 1.000000 0.00 0.0000 111.049 0.000 12 1513.69755 4.90614 1.854780 24.80 0.6121 110.359 577.489 13 −741.75658 2.20000 1.618000 63.33 0.5441 109.554 −301.969 14 250.89124 (Variable) 1.000000 0.00 0.0000 104.471 0.000 *15 399.99280 2.00000 1.816000 46.62 0.5558 53.397 −73.464 16 52.24705 9.67114 1.000000 0.00 0.0000 47.225 0.000 17 −68.98087 1.50000 1.595220 67.74 0.5442 47.360 −68.812 18 102.52955 0.80000 1.000000 0.00 0.0000 45.877 0.000 19 136.99502 7.39188 1.720467 34.70 0.5834 45.875 65.381 20 −70.89345 1.50000 1.595220 67.74 0.5442 45.622 −65.260 21 87.27916 0.20000 1.000000 0.00 0.0000 43.852 0.000 *22 61.79860 6.83810 1.720467 34.70 0.5834 43.785 69.887 23 −269.03086 2.31018 1.000000 0.00 0.0000 43.138 0.000 24 −70.70437 1.90000 1.595220 67.74 0.5442 43.311 −66.658 25 92.05492 (Variable) 1.000000 0.00 0.0000 41.842 0.000 26 465.31833 4.92170 1.595220 67.74 0.5442 49.061 143.380 27 −104.54692 0.20000 1.000000 0.00 0.0000 50.141 0.000 28 −95.23894 1.80000 1.834000 37.16 0.5775 50.133 −142.254 *29 −474.76565 0.20000 1.000000 0.00 0.0000 51.469 0.000 30 145.94554 8.21762 1.496999 81.54 0.5374 53.027 109.259 31 −85.25411 (Variable) 1.000000 0.00 0.0000 53.316 0.000 32 103.02061 5.56834 1.595220 67.74 0.5142 52.181 150.827 33 −703.36095 0.20000 1.000000 0.00 0.0000 51.803 0.000 34 89.83478 1.80000 1.720457 34.70 0.5834 50.110 −110.447 35 41.99222 0.16549 1.000000 0.00 0.0000 47.460 0.000 36 42.51067 8.55432 1.496999 81.54 0.5374 47.468 82.867 37 −1359.32426 (Variable) 1.000000 0.00 0.0000 47.086 0.000 38 (Stop) 0.00000 2.50000 1.000000 0.00 0.0000 31.098 0.000 39 −163.06739 1.60000 1.639999 60.08 0.5370 30.114 −82.140 40 78.33421 0.10000 1.000000 0.00 0.0000 29.207 0.000 41 26.40020 4.11138 1.531717 48.84 0.5630 28.721 83.119 42 61.56760 0.96556 1.000000 0.00 0.0000 27.936 0.000 43 150.41160 1.60000 1.772499 49.60 0.5521 27.930 −64.121 44 37.22289 21.33094 1.000000 0.00 0.0000 26.573 0.000 45 171.59368 1.60000 1.882997 40.76 0.5667 25.107 −34.393 46 25.81664 6.10167 1.698947 30.13 0.6029 25.391 29.502 47 −96.15077 21.91788 1.000000 0.00 0.0000 25.766 0.000 48 47.42133 2.60000 1.882997 40.76 0.5667 29.452 −74.692 *49 26.94011 3.46433 1.000000 0.00 0.0000 28.538 0.000 50 45.25765 8.84848 1.501372 56.42 0.5533 29.709 42.157 51 −37.35449 1.60000 1.882997 40.76 0.5667 30.004 −45.343 52 −526.08631 0.20000 1.000000 0.00 0.0000 31.124 0.000 53 50.27100 11.66669 1.501372 56.42 0.5533 32.437 35.502 54 −25.58199 1.60000 1.882997 40.76 0.5667 32.551 −50.512 55 −61.27756 (BF) 1.000000 0.00 0.0000 34.280 0.000 Image plane ∞ Aspherical surface data Fifteenth surface K = 9.56606e+000 A4 = −2.38525e−007 A6 = 3.05939e−010 A8 = 1.73334e−013 A10 = −4.06823e−016 A12 = 3.14889e−019 Twenty-second surface K = 9.14684e−001 A4 = 3.44432e−007 A6 = −6.79631e−010 A8 = −1.94799e−014 A10 = 4.71804e−016 A12 = 6.96922e−019 Twenty-ninth surface K = 1.77658e+001 A4 = 3.76174e−007 A6 = −3.85412e−011 A8 = 1.69970e−013 A10 = −2.14148e−016 A12 = 1.04959e−019 Fifty-second surface K = −1.07821e+000 A4 = 5.89784e−007 A6 = −3.15957e−009 A8 = 1.97960e−011 A10 = −1.60622e−013 A12 = 2.81140e−016 Various data Zoom ratio 20.00 Wide angle Intermediate Telephoto Focal length 50.00 200.00 1000.00 F number 4.50 4.50 7.50 Half angle of field 23.40 6.18 1.24 Image height 21.64 21.64 21.64 Total lens length 479.16 479.16 479.16 BF 61.37 61.37 61.37 d14 1.21 74.31 125.17 d25 141.34 55.50 0.84 d31 36.46 21.70 5.01 d37 1.62 29.12 49.61 Zoom lens unit data Unit First surface Focal length 1 1 235.00 2 15 −30.85 3 26 110.00 4 32 105.00 5 38 −110.47

Numerical Embodiment 5

Surface Effective Focal number r d nd νd θgF diameter length 1 307.55163 17.57143 1.433870 95.10 0.5373 149.996 451.344 2 −533.39025 0.70000 1.000000 0.00 0.0000 149.539 0.000 3 283.38566 19.58639 1.433870 95.10 0.5373 144.216 367.735 4 −359.52266 1.00394 1.000000 0.00 0.0000 142.980 0.000 5 −350.09799 4.00000 1.720467 34.70 0.5834 142.255 −339.417 6 833.68327 25.29114 1.000000 0.00 0.0000 138.659 0.000 7 277.14461 13.82768 1.433870 95.10 0.5373 129.141 522.598 8 −1244.99211 0.20000 1.000000 0.00 0.0000 127.470 0.000 9 188.53605 12.94197 1.433870 95.10 0.5373 120.593 430.399 10 −25989.26163 2.50000 1.720467 34.70 0.5834 118.771 −1254.775 11 943.26663 2.94687 1.000000 0.00 0.0000 116.579 0.000 12 2527.57480 8.10238 1.761821 26.52 0.6135 115.129 447.924 13 −398.00062 2.20000 1.618000 63.33 0.5441 113.597 −239.450 14 237.48185 (Variable) 1.000000 0.00 0.0000 107.043 0.000 *15 −425.16063 1.80000 1.754998 52.32 0.5476 46.002 −120.203 16 116.26240 6.91604 1.000000 0.00 0.0000 43.489 0.000 17 −77.43514 1.50000 1.595220 67.74 0.5442 41.934 −71.657 18 96.39345 6.90387 1.720467 34.70 0.5834 40.434 56.038 19 −68.17358 1.50000 1.000000 0.00 0.0000 40.005 0.000 20 −70.21381 1.50000 1.595220 67.74 0.5442 38.049 −57.436 21 67.62333 4.23715 1.720467 34.70 0.5834 35.815 92.341 22 −6881.20455 2.86458 1.000000 0.00 0.0000 35.172 0.000 23 −56.49108 1.40000 1.595220 67.74 0.5442 35.115 −59.347 24 96.05248 (Variable) 1.000000 0.00 0.0000 34.430 0.000 25 106.06442 7.16064 1.618000 63.33 0.5441 46.688 82.278 26 −95.83925 0.12492 1.000000 0.00 0.0000 46.737 0.000 27 −104.32654 1.50000 1.834000 37.16 0.5775 46.634 −110.930 *28 871.36349 0.20000 1.000000 0.00 0.0000 46.934 0.000 29 81.28697 5.70154 1.496999 81.54 0.5374 47.635 153.268 30 −1240.33801 (Variable) 1.000000 0.00 0.0000 47.512 0.000 *31 123.98329 6.47892 1.487490 70.23 0.5300 47.027 118.458 32 −106.91516 0.20000 1.000000 0.00 0.0000 46.694 0.000 33 319.00503 1.50000 1.720467 34.70 0.5834 44.905 −124.926 34 70.43254 6.03125 1.496999 81.54 0.5374 43.469 119.239 35 −369.81289 (Variable) 1.000000 0.00 0.0000 42.874 0.000 36 (Stop) 0.00000 8.63110 1.000000 0.00 0.0000 33.266 0.000 37 361.88964 1.40000 1.882997 40.76 0.5667 28.053 −31.579 38 25.98178 5.71981 1.761821 26.52 0.6135 26.443 30.235 39 −199.02059 3.00000 1.000000 0.00 0.0000 25.962 0.000 40 −331.36717 1.50000 2.003300 28.27 0.5980 23.925 −49.856 41 59.63035 30.00000 1.000000 0.00 0.0000 23.167 0.000 *42 58.84110 4.66497 1.517417 52.43 0.5564 25.147 55.540 43 −55.13321 0.75000 1.000000 0.00 0.0000 25.010 0.000 44 −66.59470 4.00000 1.882997 40.76 0.5667 24.623 −22.456 45 29.27488 6.36072 1.603420 38.03 0.5835 24.517 29.695 46 −43.08869 1.50000 1.000000 0.00 0.0000 24.791 0.000 47 −94.91780 4.20692 1.517417 52.43 0.5564 24.473 68.670 48 −26.33176 3.00000 1.834807 42.71 0.5642 24.486 −51.269 49 −71.36289 (BF) 1.000000 0.00 0.0000 25.385 0.000 Image plane ∞ Aspherical surface data Fifteenth surface K = −1.85753e+002 A4 = 8.14403e−007 A6 = 8.72314e−011 A8 = 7.71433e−013 A10 = −1.72911e−015 A12 = 1.37509e−018 Twenty-eighth surface K = 7.34242e+002 A4 = 3.16380e−007 A6 = 8.34068e−011 A8 = 3.51830e−013 A10 = 5.94163e−016 A12 = −4.65419e−019 Thirty-first surface K = −6.36723e+000 A4 = −5.33965e−007 A6 = −4.59300e−011 A8 = 3.58485e−014 A10 = 1.31143e−016 A12 = −1.64997e−019 Forty-second surface K = 3.06784e+000 A4 = 1.08776e−006 A6 = −1.98897e−009 A8 = 2.90074e−011 A10 = −1.43531e−013 A12 = 2.37788e−016 Various data Zoom ratio 30.00 Wide angle Intermediate Telephoto Focal length 50.00 500.00 1500.00 F number 4.50 5.00 10.00 Half angle of field 15.64 1.60 0.53 Image height 14.00 14.00 14.00 Total lens length 520.83 520.83 520.83 BF 70.00 70.00 70.00 d14 3.03 121.51 142.94 d24 185.06 59.90 3.00 d30 17.62 1.94 55.46 d35 2.00 24.34 6.30 Zoom lens unit data Unit First surface Focal length 1 1 270.00 2 15 −32.50 3 25 103.00 4 31 113.50 5 36 −88.23

Numerical Embodiment 6

Surface Effective Focal number r d nd νd θgF diameter length 1 296.53152 4.00000 1.712995 53.87 0.5458 142.858 −823.871 2 196.23701 1.00000 1.000000 0.00 0.0000 141.132 0.000 3 206.15767 17.70419 1.433870 95.10 0.5373 141.199 400.193 4 −1089.16753 0.20000 1.000000 0.00 0.0000 140.948 0.000 5 356.13631 4.00000 1.743198 49.34 0.5530 139.269 −277.640 6 130.41565 0.15000 1.000000 0.00 0.0000 134.928 0.000 7 129.45681 15.54802 1.433870 95.10 0.5373 135.092 446.030 8 374.92795 13.54253 1.000000 0.00 0.0000 134.873 0.000 9 155.29485 18.86311 1.433870 95.10 0.5373 135.785 339.935 10 −2973.97397 0.20000 1.000000 0.00 0.0000 135.140 0.000 11 150.08297 14.42543 1.433870 95.10 0.5373 128.939 443.558 12 656.09723 (Variable) 1.000000 0.00 0.0000 127.278 0.000 13 −1581.09064 1.80000 1.816000 46.62 0.5568 49.507 −52.360 14 44.16547 9.90829 1.000000 0.00 0.0000 44.328 0.000 15 −66.23190 1.50000 1.495999 81.54 0.5374 44.292 −134.054 16 −7582.68151 0.15000 1.000000 0.00 0.0000 44.615 0.000 17 78.57682 8.73981 1.720467 34.70 0.5834 44.922 53.821 18 −73.96482 1.50000 1.496999 81.54 0.5374 44.520 −88.827 19 111.05326 0.20000 1.000000 0.00 0.0000 42.214 0.000 20 46.38655 3.91260 1.720467 34.70 0.5834 41.294 171.759 21 71.27968 4.70907 1.000000 0.00 0.0000 40.158 0.000 22 −116.93181 1.40000 1.595220 67.74 0.5442 40.105 −76.194 23 74.84737 (Variable) 1.000000 0.00 0.0000 38.894 0.000 24 117.28808 6.98179 1.618000 63.33 0.5441 44.080 79.825 25 −83.74630 0.15000 1.000000 0.00 0.0000 44.168 0.000 26 −84.76803 1.50000 1.834000 37.16 0.5775 44.116 −98.094 *27 2888.86663 0.20000 1.000000 0.00 0.0000 44.583 0.000 28 99.34248 5.58632 1.496995 81.54 0.5374 45.190 1.39777 29 −228.91625 (Variable) 1.000000 0.00 0.0000 45.184 0.000 30 307.57238 4.08165 1.487490 70.23 0.5300 44.776 224.345 31 −169.86545 0.20000 1.000000 0.00 0.0000 44.564 0.000 32 74.84159 1.50000 1.720467 34.70 0.5834 43.061 −154.226 33 44.46471 0.85000 1.000000 0.00 0.0000 41.557 0.000 34 49.40372 6.01491 1.496999 81.54 0.5374 41.557 −1.#I0 35 0.00000 (Variable) 1.000000 0.00 0.0000 41.124 0.000 36 (Stop) 0.00000 10.52322 1.000000 0.00 0.0000 29.612 0.000 37 259.95225 1.40000 1.882997 40.76 0.5667 24.638 −55.642 33 41.41924 0.15000 1.000000 0.00 0.0000 23.824 0.000 39 32.89909 4.21323 1.805181 25.42 0.6161 23.817 39.648 40 −1471.23937 4.50275 1.000000 0.00 0.0000 23.144 0.000 41 −204.34876 1.50000 1.910820 35.25 0.5824 20.271 −31.947 42 34.31624 33.00000 1.000000 0.00 0.0000 19.376 0.000 43 63.14969 6.66912 1.496999 81.54 0.5374 30.326 63.166 44 −60.58599 5.51773 1.000000 0.00 0.0000 30.552 0.000 45 −92.46799 4.00000 1.882997 40.76 0.5667 29.451 −32.760 46 43.31702 7.95980 1.603420 38.03 0.5835 29.922 39.436 47 −49.82488 0.15000 1.000000 0.00 0.0000 30.512 0.000 48 162.75165 5.38663 1.501372 56.42 0.5533 30.317 69.768 49 −44.29892 3.00000 1.882997 40.76 0.5667 30.107 −61.901 50 −235.34177 (BF) 1.000000 0.00 0.0000 30.447 0.000 Image plane ∞ Aspherical surface data Twenty-seventh surface K = 7.88437e+003 A4 = 3.70999e−007 A6 = 2.97099e−011 A8 = −1.13196e−013 A10 = 1.01136e−016 A12 = −4.55239e−020 Various data Zoom ratio 20.00 Wide angle Intermediate Telephoto Focal length 40.00 400.00 800.00 F number 4.50 4.50 5.60 Half angle of field 21.24 2.23 1.11 Image height 15.55 15.55 15.55 Total lens length 488.14 488.14 488.14 BF 64.42 64.42 64.42 d12 2.73 113.53 127.29 d23 162.00 45.39 7.70 d29 18.69 3.86 43.33 d35 1.81 22.45 6.91 Zoom lens unit data Unit First surface Focal length 1 1 205.00 2 13 −34.00 3 24 105.00 4 30 125.00 5 36 −317.30

TABLE 1 Table 1: Values of conditional expressions (1) to (8) for Embodiments 1 to 6 Embodiment 1 2 3 4 5 6 fw 50.0 60.0 50.0 50.0 50.0 40.0 ft 1,000.0 900.0 500.0 1,000.0 1,500.0 800.0 f1 255.0 245.6 205.0 235.0 270.0 205.0 f1f 188.67 165.00 157.52 182.26 196.38 −11,562.31 f1r −536.06 −373.50 −559.16 −636.65 −518.14 194.87 β2w −0.25 −0.28 −0.26 −0.21 −0.22 −0.25 β2t −3.01 −3.33 −1.72 −1.53 −4.22 −3.51 β3w −0.93 −1.45 −2.10 −1.23 −0.78 −0.90 β3t −2.10 −2.19 −24.32 10.34 −1.30 −1.44 β4w 0.42 0.31 0.21 0.34 0.42 0.42 β4t 0.31 0.25 0.03 −0.11 0.40 0.38 β5 2.00 1.98 2.09 1.00 2.56 2.03 UD1 89.95 78.86 63.04 79.61 110.87 89.63 βcw −0.79 −0.88 −0.92 −0.42 −0.84 −0.77 βct −1.31 −1.10 −1.42 −1.17 −1.32 −1.11 βct/βcw 1.66 1.26 1.54 2.80 1.57 1.44 ft/fw 20.00 15.00 10.00 20.00 30.00 20.00 ωw 17.28 14.53 17.28 23.40 15.64 21.24 Conditional Expression (1) 0.17 0.08 0.19 0.34 0.13 0.12 (2) 3.92 3.66 2.44 4.26 5.56 3.90 (3) 64.29 57.88 32.15 46.22 107.16 51.46 (4) −0.35 −0.44 −0.28 −0.29 −0.38 −59.33 (5) 0.35 0.32 0.31 0.34 0.41 0.44 (6) −0.25 −0.20 −0.26 −0.21 −0.22 −0.25 (7) −4.95E−04 −6.40E−04 −7.37E−04 −5.07E−04 −4.78E−04 −2.78E−04 (8) −1.30E−03 −1.40E−03 −1.08E-03 −1.30E−03 −1.31E−03 −1.14E−03

(Image Pickup Apparatus)

Next, an image pickup apparatus using the zoom lens according to each embodiment as an image pickup optical system is described. FIG. 13 is a schematic diagram of a main part of an image pickup apparatus (television camera system) using the zoom lens according to each embodiment as an image pickup optical system. FIG. 13 illustrates a zoom lens 101, which is any one of the zoom lenses according to Embodiments 1 to 6.

The zoom lens 101 may be detachably mounted on a camera body 124, to thereby construct an image pickup apparatus 125. The zoom lens 101 includes a first lens unit 114, a zoom portion 115 that moves during zooming, and a lens unit 116 for imaging. Further, the zoom lens 101 includes an aperture stop SP. The lens unit 116 that does not move for zooming includes a zoom optical system IE, which is retractably insertable in an optical path.

The zoom portion 115 includes a drive mechanism for being driven in the optical axis direction. Drive units 117 and 118 such as motors electrically drive the zoom unit 115 and the aperture stop SP, respectively. Note that, the drive mechanism may be added to move all of the lens units 114, 115, and 116 or a part of each lens unit in the optical axis direction for focusing. Detectors 119 and 120 such as an encoder, a potentiometer, or a photosensor for detecting positions of the lens units in the zoom unit 115 on the optical axis and a stop diameter of the aperture stop SP. Note that, drive loci of the lens units in the zoom unit 115 may be mechanical loci by a helicoid, a cam, or the like, or electric loci by an ultrasonic motor or the like. In addition, the camera body 124 includes a glass block 109, which is equivalent to an optical filter or a color separation prism in the camera body 124. Further, the camera body 124 includes a solid-state image pickup element (photoelectrical transducer) 110, such as a CCD sensor or a CMOS sensor. The solid-state image pickup element 110 is configured to receive an object image formed by the zoom lens 101. Further, CPUs 111 and 122 control the driving of the camera body 124 and the zoom lens 101, respectively. By applying the zoom lens according to the present invention to a television camera as described above, an image pickup apparatus having high optical performance may be implemented.

While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.

This application claims the benefit of Japanese Patent Application No. 2014-094609, filed May 1, 2014, which is hereby incorporated by reference herein in its entirety. 

What is claimed is:
 1. A zoom lens, comprising, in order from an object side to an image side: a first lens unit having a positive refractive power that does not move for zooming; a second lens unit having a negative refractive power that moves during zooming; a third lens unit having a positive refractive power that moves during zooming; and at least one lens unit having a positive refractive power, wherein the following conditions are satisfied: 0.02<LN(|βct/βcw|)/LN(ft/fw)<0.50 2.0<ft/f1<7.0 20<ft/(fw×tan ωw)<120 where fw and ft represent focal lengths of the zoom lens at a wide angle end and a telephoto end, respectively, ωw represents a maximum value of a half angle of field at the wide angle end, βct and βcw represent products of lateral magnifications of lens units arranged on the image side of the third lens unit in a state in which focus is at infinity at the telephoto end and the wide angle end, respectively, and LN( ) in the conditional expression represents a natural logarithm of a numerical value in parentheses.
 2. The zoom lens according to claim 1, wherein the first lens unit includes a front lens unit having a positive refractive power and including a negative lens, and a rear lens unit having a negative refractive power and including a positive lens and a negative lens, and satisfies the following condition: −0.50<f1f/f1r<−0.20 where f1 f represents a focal length of the front lens unit, and f1 r represents a focal length of the rear lens unit.
 3. The zoom lens according to claim 1, wherein, of the lens units on the image side of the third lens unit, a lens unit that is closest to the image side comprises a lens unit having a positive refractive power that does not move for zooming.
 4. The zoom lens according to claim 1, wherein the lens units on the image side of the third lens unit comprise a fourth lens unit having a positive refractive power that moves during zooming, and a fifth lens unit having a positive refractive power that does not move for zooming.
 5. The zoom lens according to claim 1, wherein the following condition is satisfied: −0.35<β2w<−0.15 where β2 w represents a lateral magnification of the second lens unit in the state in which focus is at infinity at the wide angle end.
 6. The zoom lens according to claim 1, wherein the following expression is satisfied: −8.50×10⁻⁴<(θ2p−θ2n)/(ν2p−ν2n)<−2.00×10⁻⁴ where ν2 p and θ2 p represent average values of Abbe numbers and relative partial dispersions of convex lenses forming the second lens unit, respectively, and ν2 n and θ2 n represent average values of Abbe numbers and relative partial dispersions of concave lenses forming the second lens unit, respectively, provided that the Abbe number ν and the relative partial dispersion θ are expressed as: ν=(Nd−1)/(NF−NC) θ=(Ng−NF)/(NF−NC) where Ng represents a refractive index in a g-Line, NF represents a refractive index in an F-Line, Nd represents a refractive index in a d-Line, and NC represents a refractive index in a C-Line.
 7. The zoom lens according to claim 1, wherein the following expression is satisfied: −1.80×10⁻³<(θ1p−θ1n)/(ν1p−ν1n)<—0.80×10⁻³ where ν1 p and θ1 p represent average values of Abbe numbers and relative partial dispersions of convex lenses forming the first lens unit, respectively, and ν1 n and θ1 n represent average values of Abbe numbers and relative partial dispersions of concave lenses forming the first lens unit, respectively, provided that the Abbe number ν and the relative partial dispersion θ are expressed as: ν=(Nd−1)/(NF−NC) θ=(Ng−NF)/(NF−NC) where Ng represents a refractive index in a g-Line, NF represents a refractive index in an F-Line, Nd represents a refractive index in a d-Line, and NC represents a refractive index in a C-Line.
 8. An image pickup apparatus, comprising: a zoom lens comprising, in order from an object side to an image side: a first lens unit having a positive refractive power that does not move for zooming; a second lens unit having a negative refractive power that moves during zooming; a third lens unit having a positive refractive power that moves during zooming; and at least one lens unit having a positive refractive power, wherein the following conditions are satisfied: 0.02<LN(|βct/βw|)/LN(ft/fw)<0.50 2.0<ft/f1<7.0 20<ft/(fw×tan ωw)<120 where fw and ft represent focal lengths of the zoom lens at a wide angle end and a telephoto end, respectively, ωw represents a maximum value of a half angle of field at the wide angle end, βct and βcw represent products of lateral magnifications of lens units arranged on the image side of the third lens unit in a state in which focus is at infinity at the telephoto end and the wide angle end, respectively, and LN( ) in the conditional expression represents a natural logarithm of a numerical value in parentheses; and an image pickup element. 